Essays: Scientific, Political, & Speculative; Vol. 2 of 3: Library Edition (1891), Containing Seven Essays not before Republished, and Various other Additions.Spencer, Herbert
Philosophy
Essays: Scientific, Political, & Speculative; Vol. 2 of 3: Library Edition (1891), Containing Seven Essays not before Republished, and Various other Additions.
Spencer, Herbert
Philosophy; Political science; Science
1. Two homogeneous bodies are rubbed together and there results heat:
the interpretation being that the molar motion is transformed into
molecular motion. Here motion produces motion—the _form_ only being
changed.
2. Now of the two bodies one is replaced by a body unlike in nature to
the other, and they are again rubbed. Again a certain amount of heat
is produced: some of the molar motion is, as before, transformed into
molecular motion. But, at the same time, another part of the molar
motion is changed into—what? Surely not a fluid, a substance, a thing.
It cannot be that what in the first case produces a change of _state_,
in the second case produces an _entity_. And in the second case itself,
it cannot be that while part of the original motion becomes changed
into another species of motion, part of it becomes changed into a
species of matter.
3. Must we not say, then, that if, when the two bodies rubbed are
homogeneous, sensible motion is transformed into insensible motion,
when they are heterogeneous, sensible motion must still be transformed
into insensible motion: such difference of nature as this insensible
motion has, being consequent on the difference of nature between the
two kinds of molecules acting on one another?
4. If, when the two masses are homogeneous, those molecules which
compose the two rubbed surfaces disturb one another, and increase one
another’s oscillations; then, when the two masses are heterogeneous,
those molecules forming the two rubbed surfaces must also disturb one
another in some way—increase one another’s agitations.
5. If, when the two sets of molecules are alike in kind, the mutual
disturbance is such that they simply increase the amplitudes of one
another’s oscillations, and do this because their times correspond;
then, must it not be {187} that when they are unlike in kind, the
mutual disturbance will involve a differential action consequent on the
unlikeness of their motions? Must not the discord of the oscillations
produce a result which cannot be produced when the oscillations are
concordant—a compound form of molecular motion?
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